roseta
Last edited: August 8, 2025Rosetta
Last edited: August 8, 2025Rosetta is a set of physical-based protein folding models.
protein binding with Rosetta
- check a protein surface
- check how protein side-chains interact with the binding surface
peptide binding with Rosetta
The difficulty with this is that we don’t know what the overall tertiary structure of a group of peptides are; unlike whole protein binding.
sequence-specific DNA binding
???
more!
You take something like a trimer; you shove a peptide between each “point”, and boom structal change to a quadromer
RoseTTAFold2
Last edited: August 8, 2025RoseTTAFold2 is a three-track folding tool, which also handles multimer!
- inputs: amino acid sequence + CHEMICAL structure (WOAH! how?)
- “RF2 all-atom embedding”
- fold!
The model does really well!
application: de-novo luciferase design
- come up with the correct shaped scaffolds
- use old Rosetta to jam a residue sequence into the scaffold
- refold
application: RoseTTAFold2 in-painting
Train the model to recover the missing bits of sequence from the overall structure (i.e. training backwards), and
Rossing 1990
Last edited: August 8, 2025On the dynamics of Tuning Forks. (Rossing, Russell, and Brown 1992)
Characterizing Tuning Forks
Aluminum, tines 10mm apart. Four main groups of vibration:
- Symmetrical In-Plane
- Antisymmetrical In-Plane
- Symmetrical Out-Of-Plane
- Antisymmetrical Out-Of-Plane

(a) and (c) are in the first group; (b) is in the second group, where the fork just warps.
Deriving Tuning Forks’ Frequency
As per before, we can treat tuning forks acting in clang and fundamental modes as a good’ol fashioned cantilever beam.
rotational energy theorem
Last edited: August 8, 2025total kinetic energy
\begin{equation} KE_{rigid} = \frac{1}{2} M{V_{cm}}^2 + \frac{1}{2} I_{CM}{\omega_{CM}}^2 \end{equation}
torque from gravity
For even non rigid bodies, the following follows:
\begin{equation} \vec{\tau}_g = \vec{R}_{CM} \times M\vec{g} \end{equation}
Actually, this follows for any \(f\) (like \(g\)) evenly applied across point masses.
potential energy
\begin{equation} \Delta PE_g = mg\Delta h \end{equation}
where, \(\Delta h\) is the travel of center of mass. Regardless of whether or not its point.